Optical recording medium, manufacturing method for optical recording medium, information recording/reproducing method and information recording/reproducing device

ABSTRACT

An optical recording medium is capable of preventing a back focus at the face thereof and reducing the interference between beams reflected by each recording surface, thereby improving the quality of a servo signal and a reproductive signal. In a disk having (N-1) layers if N is a natural number (more than three), if a cover-layer thickness and intermediate-layer thicknesses are d 1 , d 2 , . . . dN, then a difference of 1 μm or above is set between the sum of di to dj and the sum of dk to dm for arbitrary natural numbers i, j, k, m (i≦j≦k≦m≦N). If the refractive indexes are different from a standard value or different for each layer, the thickness of each layer is converted on the basis of the spread width of light according to the thickness.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an optical recording medium irradiated with light to record or reproduce information. Particularly, it relates to a layer-interval structure of an optical recording medium having three or more information recording surfaces, and a method or a device for reproducing information on the multilayer optical recording medium or recording information therein.

2. Description of the Background Art

A high-density and large-capacity optical information recording medium is on the market—typically, an optical disk such as a DVD or a BD. The optical disk has recently become increasingly popular as a recording medium for recording an image, music or computer data. In order to increase the recording capacity, an optical recording medium having a plurality of recording layers has been offered, as described in Japanese Patent Laid-Open Publication No. 2001-155380 or Japanese Patent Laid-Open Publication No. 2008-117513.

FIG. 13 shows a conventional configuration of an optical recording medium and an optical pickup. A divergent beam 70 emitted from a light source 1: transmits a collimating lens 53 provided with a spherical-aberration correcting means 93; is incident upon a polarization beam splitter 52 and transmits it; transmits a quarter-wave plate 54 to convert into a circularly polarized beam; thereafter, is converted into a convergent beam by an objective lens 56; transmits a transparent substrate of an optical recording medium 401 to concentrate upon any of recording surfaces 401 a, 401 b, 401 c and 401 d formed inside of the optical recording medium 401. The objective lens 56 is designed in such a way that the spherical aberration is zero in the middle depth position between the first recording surface 401 a and the fourth recording surface 401 d. The spherical-aberration correcting means 93 moves the collimating lens 53 in the optical-axis directions to thereby remove a spherical aberration generated when a beam converges upon each recording surface 401 a, 401 b, 401 c, 401 d.

The objective lens 56 is provided with an aperture portion 55 restricting the aperture thereof and has a numerical aperture NA of 0.85. The beam 70 reflected by the fourth recording surface 401 d transmits the objective lens 56 and the quarter-wave plate 54 to convert into a linearly polarized beam different by an angle of 90 degrees from the outward path; thereafter, is reflected by the polarization beam splitter 52; transmits a condensing lens 59 to convert into a convergent beam; is given an astigmatism through a cylindrical lens 57; and is incident upon a photodetector 320.

The photodetector 320 includes four light-receiving portions (not shown) each outputting an electric-current signal according to the quantity of received light. Each electric-current signal is used for generating a focus error (FE) signal in an astigmatism method, a tracking error (TE) signal in a push-pull method and an information (RF) signal recorded in the optical recording medium 401. The FE signal and the TE signal are amplified to a desired level and compensated for phase, and thereafter, are supplied to actuators 91 and 92 for focus and tracking control.

Herein, a problem arises if thicknesses t1 to t4 are all equal, as follows. For example, in order to execute recording and reproduction for the fourth recording surface 401 d, the beam 70 is concentrated on there, and then, a part of the beam 70 is reflected by the third recording surface 401 c. Since the distance between the third recording surface 401 c and the fourth recording surface 401 d is equal to the distance between the third recording surface 401 c and the second recording surface 401 b, the part of the beam 70 reflected by the third recording surface 401 c forms an image on the back side of the second recording surface 401 b, and the reflected beam by the second recording surface 401 b is reflected again by the third recording surface 401 c and gets mixed with a reflected beam from the fourth recording surface 401 d which should be naturally read. Further, since the distance between the second recording surface 401 b and the fourth recording surface 401 d is also equal to the distance between the second recording surface 401 b and a face 401z of the optical recording medium 401, a part of the beam 70 reflected by the second recording surface 401 b forms an image on the back side of the face 401 z of the optical recording medium 401, and the reflected beam by the face 401 z is reflected again by the second recording surface 401 b and gets mixed with the reflected beam from the fourth recording surface 401 d which should be naturally read. This causes the problem of super imposing multiple reflected beams from images formed on the back sides of other layers on the reflected beam from the fourth recording surface 401 d which should be naturally read to thereby hinder the recording/reproduction. The mixed beams tend to interfere and form a brightness distribution through interference on a light-receiving element, and the brightness distribution varies according to the change in the phase difference between the reflected beam from the fourth recording surface 401 d and a reflected beam from another layer which is caused by a slight dispersion of intermediate-layer thicknesses inside of the face of an optical disk, thereby significantly deteriorating the quality of a servo signal and a reproductive signal. In the specification, this is below called the back-focus problem.

In order to prevent this, a method is disclosed of gradually lengthening the distance between each recording layer one by one from the face 401 z of the optical recording medium 401 in such a way that no image is formed on the back side of the second recording surface 401 b or the back side of the face 401 z at the same time that the beam 70 is concentrated on the fourth recording surface 401 d from which reading should be naturally executed (refer to Japanese Patent Laid-Open Publication No. 2001-155380). Herein, the thicknesses t1 to t4 each have a manufacturing dispersion of ±10 μm, and even if they are widely dispersed, each thickness t1 to t4 needs to have a different distance, thereby setting the difference in distance, for example, to 20 μm. In this case, t1=40 μm, t2=60 μm, t3=80 μm and t4=100 μm, then a total thickness t (=t2+t3+t4) from the first recording surface 401 a to the fourth recording surface 401 d becomes 240 μm.

If the thickness of a cover layer between the face and the first recording surface 401 a is equal to the thickness between the fourth recording surface 401 d and the first recording surface 401 a, then a beam reflected by the fourth recording surface 401 d is focused at the face and reflected from there, is reflected again by the fourth recording surface 401 d, and thereafter, is led to the light-receiving portions. Because of the back focus at the face, this luminous flux does not have information such as a pit and a mark contained in a back-focus luminous flux on another recording layer. However, if there are a large number of recording layers, the quantity of light returning from the recording layers decreases to thereby heighten the reflectance of the face relatively. Accordingly, interference with a luminous flux on a reproduction layer occurs likewise, thereby significantly deteriorating the quality of a servo signal and a reproductive signal.

Taking the above problems into account, Japanese Patent Laid-Open Publication No. 2008-117513 suggests the distance between recording layers in an optical disk and discloses a structure as follows.

An optical recording medium includes four information recording surfaces—first to fourth information recording surfaces in order from the face of the optical recording medium. The distance between the face and the first information recording surface is 47 μm or below, and the intermediate-layer thickness between each information surface from the first information recording surface to the fourth information recording surface is a combination of 11-15 μm, 16-21 μm, and 22 μm or above. The distance between the face and the fourth information recording surface is 100 μm.

The distance between the face and the first information recording surface is 47 μm or below and the distance between the face and the fourth information recording surface is 100 μm.

In an optical disk system, a beam of light is incident upon the face of an optical disk and reflected by a recording surface, and the reflected beam is detected. Hence, an influence is also given by the refractive index of a transparent material transmitting the beam from the face to an optical-disk surface. In the disk structures of Japanese Patent Laid-Open Publication No. 2001-155380 and Japanese Patent Laid-Open Publication No. 2008-117513, however, neither an examination nor a description is given about the refractive index of a transparent material, and thus, an effect given by the refractive index is not considered at all.

SUMMARY OF THE INVENTION

It is an object of the present invention to provide an optical disk (optical recording medium) capable of preventing a back focus at the face thereof and reducing the interference between beams reflected by each recording surface in consideration of a refractive index, and having a multilayer disk structure of three, four or more recording layers capable of widening the distance between the face and the recording layer closest to the face to the maximum.

The other objects, characteristics and superior points of the present invention will be sufficiently understood in the following description. Further, the advantages of the present invention will be obvious in the following description with reference to the attached drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic view showing a configuration of an optical recording medium and an optical pickup according to the present invention.

FIG. 2 is a schematic view showing a layer formation of the optical recording medium according to the present invention.

FIG. 3 is a schematic view showing the problems to be solved by the invention and a beam reflected by an information recording surface for recording and reproduction.

FIG. 4 is a schematic view showing the problems to be solved by the invention and a beam reflected by surfaces other than the information recording surface for recording and reproduction.

FIG. 5 is a schematic view showing the problems to be solved by the invention and a beam reflected by surfaces other than the information recording surface for recording and reproduction.

FIG. 6 is a schematic view showing the problems to be solved by the invention and a beam reflected by surfaces other than the information recording surface for recording and reproduction.

FIG. 7 is a graphical representation showing a relationship between an FS-signal (light-quantity) amplitude and the difference in thickness between two interlayer distances of the optical recording medium.

FIG. 8 is a graphical representation showing a relationship between the substrate thickness of the optical recording medium and a jitter.

FIG. 9 is a schematic view showing a layer formation of the optical recording medium according to the present invention.

FIG. 10 is a graphical representation showing the refractive-index dependency of a coefficient for converting a shape thickness into a standard refractive index.

FIG. 11 is a graphical representation showing a conversion coefficient of a thickness corresponding to a standard refractive index into a shape thickness at an actual refractive index.

FIG. 12 is a schematic view of an optical information device according to an embodiment of the present invention.

FIG. 13 is a schematic view showing a configuration of an optical recording medium and an optical pickup head unit in a conventional optical information device.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS OF THE INVENTION

An optical recording medium according to each embodiment of the present invention will be below described with reference to the attached drawings.

First Embodiment

An embodiment of the present invention will be below described with reference to FIG. 1 and FIG. 2.

FIG. 1 shows a configuration of an optical information device according to the present invention. An optical pickup head unit 201 (or an optical pickup) irradiates an optical recording medium 40 with a blue laser beam having a wavelength λ of 405 nm or so to thereby reproduce a signal recorded in the optical recording medium 40. The optical recording medium 40 is formed with, as an example, four information recording surfaces—first to fourth information recording surfaces 40 a, 40 b, 40 c and 40 d in order from the face of the optical recording medium 40, as shown in FIG. 2. The optical recording medium 40 is also formed with a cover layer 42, a first intermediate layer 43, a second intermediate layer 44 and a third intermediate layer 45. The thickness of the cover layer 42 (substrate from a face 40 z to the first information recording surface 40 a) is t1; the thickness of the first intermediate layer 43 (substrate from the first information recording surface 40 a to the second information recording surface 40 b) is t2; the thickness of the second intermediate layer 44 (substrate from the second information recording surface 40 b to the third information recording surface 40 c) is t3; and the thickness of the third intermediate layer 45 (substrate from the third information recording surface 40 c to the fourth information recording surface 40 d) is t4. Further, the distance between the face 40 z and the first information recording surface 40 a is d1 (≈t1); the distance between the face 40 z and the second information recording surface 40 b is d2 (≈t1+t2); the distance between the face 40 z and the third information recording surface 40 c is d3 (≈t1+t2+t3); and the distance between the face 40 z and the fourth information recording surface 40 d is d4 (≈t1+t2+t3+t4).

Herein, problems will be described in the case of four information recording surfaces. Firstly, interference caused by beams reflected from multiple surfaces will be explained with reference to FIGS. 3 to 7. A luminous flux concentrated for reproduction or recording shown in FIG. 3 branches off to several light beams as follows:

a beam 70 concentrated on a reproduction or recording surface as shown in FIG. 3,

a beam 71 (back-focus beam to a recording layer) reflected by the third information recording surface 40 c, focused on the second information recording surface 40 b and reflected from there, and reflected again by the third information recording surface 40 c, as shown in FIG. 4,

a beam 72 (back-focus beam to the face) reflected by the second information recording surface 40 b, focused on the face and reflected from there, and reflected again by the second information recording surface 40 b, as shown in FIG. 5, and

a beam 73 reflected by the information recording surfaces 40 c, 40 a and 40 b in this order without being focused on any information recording surface, as shown in FIG. 6.

To begin with, an examination is made of the case where the cover layer 42, the first intermediate layer 43, the second intermediate layer 44 and the third intermediate layer 45 all have the same refractive index—a common refractive index no.

For example, if t4=t3, then upon being emitted from the face 40 z, the beam 70 and the beam 71 pass along the same optical path and thereby are incident with the same flux diameter upon the photodetector 320. Similarly, if t4+t3=t2+t1, and if t2=t4, then upon being emitted from the face 40 z, the beam 70 and the beam 72, and the beam 70 and the beam 73, respectively, pass along the same optical path and thereby are incident with the same flux diameter upon the photodetector 320. Herein, the beams 71 to 73 as multiple-surface reflected beams are less intense than the beam 70, however the contrast of interference depends upon not the intensity of light but the amplitude light-intensity ratio of light. The amplitude of light is equal to the square root of the intensity of light, thereby enlarging the contrast of interference even if there is a slight difference in the intensity of light. Upon being incident with the same flux diameter on the photodetector 320, beams are largely affected by interference, and thus, a slight change in the interlayer thickness significantly varies the quantity of light received by the photodetector 320, thereby making it hard to detect a stable signal.

FIG. 7 shows the FS-signal (total light-intensity) amplitude relative to the difference in the interlayer thickness if the light-intensity ratio of the beam 70 to the beam 71, the beam 72 or the beam 73 is 100:1 and the refractive indexes of the cover layer 42 and the first intermediate layer 43 are approximately 1.6 (1.57) equal to each other. The abscissa axis is the difference in the interlayer thickness and the ordinate axis is the FS-signal amplitude. Assuming that there is no reflection from multilayer light, the graph shows values obtained by normalizing only the beam 70 using the DC light quantity received by the photodetector 320. As can be seen from FIG. 7, the FS signal fluctuates sharply as the interlayer-thickness difference comes within approximately 1 μm.

In the same way as the beam 72 of FIG. 5, even when the difference between the thickness t1 of the cover layer 42 and the total thickness (t2+t3+t4) of the intermediate layers 43 to 45 becomes 1 μm or below, the problem arises such as fluctuations in the FS signal and the like.

As a second problem, if the interlayer distance between information recording surfaces is too narrow, the influence of crosstalk from each adjacent information recording surface is produced, thereby requiring that the interlayer distance should be set to a predetermined value or above. Accordingly, the interlayer thickness is studied to thereby determine a minimum interlayer thickness. FIG. 8 shows a relationship between the thickness between each recording layer in a disk whose recording layers have a reflectance substantially equal to each other and a jitter. The refractive indexes thereof are approximately 1.6. In FIG. 8, the abscissa axis is the thickness between layers and the ordinate axis is a jitter value. As the interlayer thickness narrows, the jitter deteriorates—begins to increase from approximately 10 μm and rises sharply below this interlayer thickness, thereby meaning that 10 μm is most suitable as the minimum value of the interlayer thickness.

A configuration of the optical recording medium 40 according to the embodiment of the present invention will be described with reference to FIG. 2. In this embodiment, in order to solve an adverse effect by a beam reflected from another layer or the face, taking the dispersion of thicknesses in production into consideration, a four-layer disk structure is set to secure the following conditions.

Condition {circle around (1)}: securing 1 μm or above as the difference between the thickness t1 of the cover layer 42 and the total thickness (t2+t3+t4) of the intermediate layers 43 to 45.

|t1−(t2+t3+t4)≧1 μm.

Condition {circle around (2)}: securing 1 μm or above as the difference between any two values of t1, t2, t3 and t4.

Condition {circle around (3)}: securing 1 μm or above as the difference between the sum (t1+t2) of the thickness t1 of the cover layer 42 and the thickness t2 of the first intermediate layer 43 and the sum (t3+t4) of the thickness t3 of the second intermediate layer 44 and the thickness t4 of the third intermediate layer 45.

Although there are some other layer-thickness combinations, they are omitted because they need no considering when a thickness of a cover layer is set to a value approximate to t2+t3+t4.

The above description is a specific example of the four-layer disk structure. However, in the case of a three-layer disk shown in FIG. 9, the conditions are as follows:

Condition {circle around (1)}: securing 1 μm or above as the difference between the thickness t1 of a cover layer 32 and the total thickness (t2+t3) of the intermediate layers 33 and 34.

t1−(t2+t3)≧1 μm, and

Condition {circle around (2)}: securing 1 μm or above as the difference between any two values of t1, t2 and t3.

More generally, in a disk having (N-1) layers (N is a natural number more than three), the above conditions are generally to set the difference between the sum of di to dj and the sum of dk to dm for arbitrary natural numbers i, j, k, m (i≦j≦k≦m≦N) to 1 μm or above if a cover-layer thickness and intermediate-layer thicknesses are d1, d2, . . . dN. The cover-layer thickness is the distance between the face of an optical recording medium and the information recording surface closest thereto, thereby similarly meaning that the distance between the face of the optical recording medium and the information recording surface second closest thereto is d2, the distance between the face of the optical recording medium and the information recording surface third closest thereto is d3, the distance between the face of the optical recording medium and the information recording surface fourth closest thereto is d4, . . . .

Moreover, all the intermediate-layer thicknesses ≧10 μm in response to the second problem.

So far, the refractive indexes are considered to be equal to a standard value and constant, however, a description will be below given about the case where the refractive indexes are different from a standard value or different for each layer. In the first problem, a back focus occurs because a signal beam and a beam reflected by another layer are similar in size or shape on a photodetector. A back focus can be avoided when the difference in focal position between a signal beam and a beam reflected by another layer must be 1 μm or above in the optical-path directions on the side of the optical recording medium if the refractive indexes are approximately 1.6. In the second problem, adjacent-layer crosstalk occurs when the defocus quantity of a signal beam is below 10 μm on an adjacent track if the refractive indexes are approximately 1.6 μm. The defocus quantity is essential and is equivalent to the size of a beam reflected by another layer or a virtual image of a beam reflected by another layer in a position where a signal beam forms a focal point. The radius thereof is set as RD. A beam reflected by another layer which has the size of RD is projected on to a photodetector, and thereby, the size of interference or crosstalk depends upon the size of RD. The size RD can be said to be a light spread width according to a thickness. We found out that in order to avoid a back focus or crosstalk if a refractive index is different from no=1.6, conditions should be devised for equating the defocus quantity or the size of a beam reflected by another layer or a virtual image of a beam reflected by another layer. In other words, the layer thickness can also be converted on the basis of the spread width of a beam according to the thickness.

When the shape thickness of a part having a refractive index nr is dr, conditions for producing the same defocus (the size of a beam reflected by another layer or a virtual image of a beam reflected by another layer) as when the shape thickness of a part having a refractive index no is do is as follows:

NA=nr·sin(θr)=no·sin(θo)   (1) and

RD=dr·tan(θr)=do·tan(θo)   (2).

Herein, NA is a numerical aperture when a beam of light converged on the optical recording medium by an objective lens 56, and for example, NA=0.85 or so. 0r and 0o are a convergent angle of a beam of light inside of a substance having each refractive index, respectively, and sin and tan are a sine function and a tangent function, respectively.

From the expression (1),

θr=arc sin(NA/nr), θo=arc sin(NA/no)   (3).

Herein, arc sin is an inverse sine function.

From the expression (2),

do=dr·tan(θr)/tan(θo)   (4) or

dr=do·tan(θo) /tan(θr)   (5).

When the shape thickness of a part having the refractive index nr is dr, in order to derive an equivalent thickness thereof corresponding to the refractive index no, do can be calculated in the expression (4).

Further, in order to equate the shape thickness dr of a part having the refractive index nr with the thickness do corresponding to the refractive index no, dr can be calculated in the expression (5).

FIG. 10 shows the coefficient part of the expression (4), or tan(θr)/tan(θo), as a function of the refractive index nr, and FIG. 11 shows the coefficient part of the expression (5), or tan(θo)/tan(θr), as a function of the refractive index nr.

If the refractive index of a predetermined layer is nr(min)≦nr≦nr(max), then in terms of the thickness dr of a part having the refractive index nr, θr(min)=arc sin(NA/nr(min)) and θr(max)=arc sin(NA/nr(max)) are set, and in the same way, the thickness range of an intermediate layer is determined in the expression of dr=do·tan(θo)/tan(θr).

A specific example is given of the relationship between a cover-layer thickness do1 of the above four-layer disk and the sum of the intermediate-layer thicknesses d2 to d4. If the refractive indexes are all no or 1.6 and do1 is 54 μm, d2 is 10 μm, d3 is 21 μm and d4 is 19 μm, then the sum of the intermediate-layer thicknesses d2 to d4 is 50 μm and different by 4 μm than do1, thereby securing 1 μm or above.

However, if the refractive index nr of the cover layer is 1.7, the situation differs even though a shape thickness d1 r of the cover layer is 54 μm which is the same as the above. In order to convert d1 r into the thickness d1 in the case where the refractive index is the standard value no, it can be seen from the expression (3) and the expression (4) or FIG. 10 that 0.921 should be multiplied. The thickness d1=0.921×d1 r=49.7 μm, which is below 50 μm as the sum of the intermediate-layer thicknesses d2 to d4. In contrast, in order to realize approximately d1=51 μm for securing 1 μm as the difference between thickness of cover layer and the sum of the intermediate-layer thicknesses d2 to d4, it can be seen from the expression (3) and the expression (5) or FIG. 11 that 1.086 should be multiplied. In other words, the calculation of d1 r=51×1.086≈55.4 μm should be made, thereby suggesting that the shape cover-layer thickness d1 r of the cover layer should be 55.4 μm or above in the case of the refractive index 1.7. This example is merely a predetermined illustration and thus the present invention is not shackled by this value.

Furthermore, in terms of how to determine d1 to dN, the above method is capable of reducing the influence of multilayer stray light possibly produced in a multilayer optical recording medium. Instead of this determining method, however, the present invention can also be applied to an optical recording medium having d1 to dN determined by another method.

Moreover, the thickness of an intermediate layer needs to fulfill specified conditions from another viewpoint. In order to stabilize a focus jump, it is desirable that the thickness of an intermediate layer is within a specified range from a standard value. The focus jump is a motion for shifting the focal position from a recording layer to another recording layer. In order to stably obtain a focus error signal in a layer toward which a focus jump is made, desirably, the quality of a focus error signal should be improved in the layer by moving the collimating lens 53 or executing another such operation before the focus jump. For this purpose, the difference in spherical aberration between the recording layers should be within a specified range.

A difference in the refractive index varies the length of a spherical aberration despite the same thickness, and thus, it is desirable that a target value or a specified tolerance for the thickness of an intermediate layer is also set in such a way that the spherical-aberration length comes within a specified range.

In addition, the present invention is not limited to any of a writable type, a write-once read-multiple type and a ROM type, and thus, can be applied to information recording media of various types.

FIG. 12 shows an optical information device making a focus jump.

The optical recording medium 40 is placed on a turntable 182 and rotated by a motor 164. The optical pickup head unit 201 described earlier is coarsely moved up to a track where desired information exits on the optical disk by an optical-head drive unit 151.

In response to the positional relation to the optical recording medium 40, the optical pickup head unit 201 sends a focus error signal or a tracking error signal to an electric circuit 153. In response to this signal, the electric circuit 153 sends a signal for finely moving an objective lens to the optical pickup head unit 201. In accordance with this signal, the optical pickup head unit 201 executes focus control or tracking control for the optical disk, and reads, writes (records) or erases information. The procedure for a focus jump is controlled mainly by the circuit 153.

With respect to the above optical information medium according to the present invention, the optical information device according to this embodiment moves the collimating lens 53 or executes another such operation before a focus jump to thereby correct a spherical aberration produced in an intermediate layer at which the jump is to be made and thereafter shifts the focal position, thereby improving the quality of a focus error signal in a layer toward which the jump is made to stabilize the focus jump.

An optical disk (=optical recording medium) according to the present invention is manufactured based on the following structures or manufacturing methods.

A first manufacturing method for an information recording medium according to the present invention is a manufacturing method for an optical recording medium which has information recording surfaces in (N-1) layers if N is a natural number (more than three), in which: if a cover-layer thickness and intermediate-layer thicknesses are d1, d2, . . . dN, then a difference DFF between the sum of di to dj and the sum of dk to dm for arbitrary natural numbers i, j, k, m (i≦j≦k≦m≦N) is 1 μm or above; and the difference DFF is calculated by converting a shape thickness dr of a part having a refractive index nr different from a standard value no into a thickness do corresponding to the refractive index no which generates the same light-beam spread width as a light-beam spread width at the thickness dr.

Furthermore, a second manufacturing method for an information recording medium according to the present invention is a manufacturing method in which further, if NA is a numerical aperture when light converged on the optical recording medium by an objective lens, θr and θo are a convergent angle of light inside of a substance having the refractive index nr and no, respectively, and sin and tan are a sine function and a tangent function, respectively, then the thickness dr of the part having the refractive index nr is converted into the thickness do of the refractive index no in relational expressions:

θr=arc sin(NA/nr), θo=arc sin (NA/no) and

do=dr·tan(θr)/tan(θo).

Moreover, a third manufacturing method for an information recording medium according to the present invention is a manufacturing method for an optical recording medium which has information recording surfaces in (N-1) layers if N is a natural number (more than three), in which: if a cover-layer thickness and intermediate-layer thicknesses are d1, d2, . . . dN, then a difference DFF between the sum of di to dj and the sum of dk to dm for arbitrary natural numbers i, j, k, m (i≦j≦k≦m≦N) is 1 μm or above; and a target value for a shape thickness dr of a part having a refractive index nr different from a standard value no is obtained by calculating a thickness do corresponding to the refractive index nr which generates the same light-beam spread width as a light-beam spread width at the thickness do corresponding to the refractive index no.

In addition, a fourth manufacturing method for an information recording medium according to the present invention is a manufacturing method in which further, if NA is a numerical aperture when light converged on the optical recording medium by an objective lens, θr and θo are a convergent angle of light inside of a substance having the refractive index nr and no, respectively, and arc sin and tan are an inverse sine function and a tangent function, respectively, then the thickness do of the part having the refractive index no is converted into the thickness dr of the refractive index nr in relational expressions:

θr=arc sin(NA/nr), θo=arc sin(NA/no) and

dr=do·tan(θo)/tan(θr).

Furthermore, a fifth manufacturing method for an information recording medium according to the present invention is a manufacturing method in which in the first to fourth manufacturing methods, the intermediate-layer thickness and the refractive index are set in such a way that a spherical aberration is within a specified range.

Moreover, an optical recording medium according to the present invention is an optical recording medium which has three or more recording layers manufactured by the first to fifth manufacturing methods.

In addition, an optical head unit according to the present invention is an optical information device which includes a motor rotating an optical disk, and an electric circuit which receives a signal obtained from the optical head unit and controls and drives the motor, an objective lens or a laser light source, in which for the optical information medium according to the present invention, prior to a focus jump, the electric circuit corrects a spherical aberration generated on an intermediate layer at which the focus jump is to be made and thereafter moves the focal position, thereby improving the quality of a focus error signal in a layer toward which the focus jump is made.

The optical recording medium according to the present invention is capable of preventing a back focus at the face thereof and reducing the interference between beams reflected by each recording surface, thereby improving the quality of a servo signal and a reproductive signal. A guide to designing a thickness according to a refractive index in the optical recording medium becomes obvious, thereby specifically clarifying a guide to the creation of a product.

The multilayer optical disk (optical recording medium) according to the present invention is capable of, even if the refractive index of a cover layer or an intermediate layer is different from a standard value, then minimizing the influence of light reflected by a layer when reproduction is executed for any other layer, thereby reducing the effect on a servo signal and a reproductive signal at an optical head.

This makes it possible to provide an optical disk capable of obtaining a high-quality reproductive signal, having a large capacity and being easily compatible with an existing disk.

Herein, the specific implementation or embodiments given in the section of DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS OF THE INVENTION merely clarify the contents of an art according to the present invention, and thus, without being limited only to the specific examples and interpreted in a narrow sense, numerous variations can be implemented within the scope of the spirit of the present invention and the following claims. 

1. A manufacturing method for an optical recording medium which has information recording surfaces in (N-1) layers if N is a natural number (more than three), wherein: if a cover-layer thickness and intermediate-layer thicknesses are d1, d2, . . . dN, then a difference DFF between the sum of di to dj and the sum of dk to dm for arbitrary natural numbers i, j, k, m (i≦j≦k≦m≦N) is 1 μm or above; and the difference DFF is calculated by converting a shape thickness dr of a part having a refractive index nr different from a standard value no into a thickness do corresponding to the refractive index no which generates the same light-beam spread width as a light-beam spread width at the thickness dr.
 2. The manufacturing method for an optical recording medium according to claim 1, wherein if NA is a numerical aperture when light converged on the optical recording medium by an objective lens, θr and θo are a convergent angle of light inside of a substance having the refractive index nr and no, respectively, and sin and tan are a sine function and a tangent function, respectively, then the thickness dr of the part having the refractive index nr is converted into the thickness do of the refractive index no in relational expressions: θr=arc sin(NA/nr), θo=arc sin(NA/no) and do=dr·tan(θr)/tan(θo).
 3. A manufacturing method for an optical recording medium which has information recording surfaces in (N-1) layers if N is a natural number (more than three), wherein: if a cover-layer thickness and intermediate-layer thicknesses are d1, d2, . . . dN, then a difference DFF between the sum of di to dj and the sum of dk to dm for arbitrary natural numbers i, j, k, m (i≦j≦k≦m≦N) is 1 μm or above; and a target value for a shape thickness dr of a part having a refractive index nr different from a standard value no is obtained by calculating a thickness do corresponding to the refractive index nr which generates the same light-beam spread width as a light-beam spread width at the thickness do corresponding to the refractive index no.
 4. The manufacturing method for an optical recording medium according to claim 3, wherein if NA is a numerical aperture when light converged on the optical recording medium by an objective lens, θr and θo are a convergent angle of light inside of a substance having the refractive index nr and no, respectively, and arc sin and tan are an inverse sine function and a tangent function, respectively, then the thickness do of the part having the refractive index no is converted into the thickness dr of the refractive index nr in relational expressions: θr=arc sin(NA/nr), θo=arc sin(NA/no) and dr=do˜tan(θo)/tan(θr).
 5. The manufacturing method for an optical recording medium according to claim 1, wherein the intermediate-layer thickness and the refractive index are set in such a way that a spherical aberration is within a specified range.
 6. An optical recording medium which has three or more recording layers manufactured by the manufacturing method for an optical recording medium according to claim
 1. 7. An optical information device which executes reproduction or recording for the optical recording medium according to claim 6, comprising: an optical head unit; a motor rotating an optical disk; and an electric circuit which receives a signal obtained from the optical head unit and controls and drives the motor, an objective lens or a laser light source, wherein prior to a focus jump, the electric circuit corrects a spherical aberration generated on an intermediate layer at which the focus jump is to be made and moves a focal position.
 8. The manufacturing method for an optical recording medium according to claim 3, wherein the intermediate-layer thickness and the refractive index are set in such a way that a spherical aberration is within a specified range.
 9. An optical recording medium which has three or more recording layers manufactured by the manufacturing method for an optical recording medium according to claim
 3. 10. An optical information device which executes reproduction or recording for the optical recording medium according to claim 9, comprising: an optical head unit; a motor rotating an optical disk; and an electric circuit which receives a signal obtained from the optical head unit and controls and drives the motor, an objective lens or a laser light source, wherein prior to a focus jump, the electric circuit corrects a spherical aberration generated on an intermediate layer at which the focus jump is to be made and moves a focal position. 